An electron with mass \( m \) and charge \( q \) is in the spin up state
\[
\begin{pmatrix} 1 \\ 0 \end{pmatrix}
\]
at time \( t = 0 \). A constant magnetic field is applied along the \( y \)-axis,
\( \mathbf{B} = B_0 \hat{j} \),
where \( B_0 \) is a constant. The Hamiltonian of the system is
\[
H = -\hbar \omega \sigma_y,
\quad \text{where} \quad \omega = \frac{q B_0}{2m} < 0
\quad \text{and} \quad
\sigma_y =
\begin{pmatrix}
0 & -i \\
i & 0
\end{pmatrix}.
\]
The minimum time after which the electron will be in the spin down state along the \( x \)-axis, i.e.,
\[
\frac{1}{\sqrt{2}} \begin{pmatrix} 1 \\ -1 \end{pmatrix},
\]
is: